The conductivities of solid solutions which contained 10mol% of a rare-earth oxide were measured (table 147) in order to determine the form of the temperature variation. It was found that the Arrhenius plots were broken straight lines, with a number of linear sections which depended upon the nature of the added ion. There was a decrease in the number of linear segments, and a shift of the low-temperature break towards higher temperatures, as the radius and polarizability of the rare-earth ion increased (see entries for ZrO2-Gd2O3, ZrO2-Ho2O3, ZrO2-Nd2O3, ZrO2-Sc2O3, ZrO2-Y2O3 and ZrO2-Yb2O3).
A.N.Vlasov: Elektrokhimiya, 1989, 25[5], 699-702
Table 147
Ionic Conduction Parameters for ZrO2-10mol%Lu2O3
Temperature (K) | ln[o (SK/cm)] | E (kJ/mol) |
1770-1500 | 5.04 | 65 |
1500-1230 | 5.24 | 70 |
1230-1000 | 5.80 | 83 |
1000-840 | 6.21 | 91 |
840-720 | 7.04 | 104 |
< 720 | 7.45 | 110 |
Ho: ionic radius = 0.0861, polarizability = 0.0013